长江口外海流结构及其季节变化

为考察长江三峡工程对河口区生态环境的影响，有必要探讨长江径流量的季节变化对河口区及口外陆架区流场结构的影响。在“长江三峡工程对长江口区流场的影响”的一文(本集)中，作者己着重探讨了三峡工程的流量调节方案将给长江口区流场带来的可能影响。本文试图从长江径流量的季节变化来分析长江口外陆架海域海流结构的季节变化，从而为三峡工程流量调节方案的设计提供某些依据。 关于长江口区及其邻近陆架海域的海流结构问题，根据实测海流资料所作的分析，迄今为止，主要限于洪水季节(即夏季)(乐肯堂，1987，1986，1984;赵保仁，1982;上海航道局设计研究所，1978;中国科学院海洋研究所，1977;华东师范大学地理系河口海岸研究室，1975,1973; Le Kentang，1986；Cannon, et al. , 1983; Beardsley et al.，1983)。长江口区枯水季节(冬季)的海流结构曾已讨论(Le Kentang, 1988)。至于春、秋两季，迄今尚未见有专题论述。本文将根据已收集到的实测余流资料(其中包括1959-1976年的资料，1980-1981年间的中美联合考察资料和1985-1986年的专题调查资料)，结合有关的水文观测资料，对本区各个季节余流的结构作一初步的分析。     

基于浮标观测的长江口外海流特征分析

为了揭示长江口外海域海流的特征及其季节和垂向变化规律,于2006年8月1日-2007年7月31日在长江口外海域（平均水深约46.0m）利用大型浮标进行了1年的分层海流流速流向观测。结果表明：（1）该海域海流为顺时针方向的旋转流,在垂向上流向较一致,季节变化不显著。（2）长江口外海域水平流速总体较大,夏季表层最大流速为128.5cm/s,冬季最大表层流速为105.5cm/s;垂线平均流速相近（差异<8.0 cm/s）,夏季流速最大为47.0cm/s,冬季为40.8cm/s。小潮的平均流速为26.5cm/s,大潮平均流速为小潮的2倍。（3）剖面各层流速垂向差异明显,最大流速出现在表层（春季和冬季）或次表层（夏季和秋季）,最小流速均出现在底层;各层的最大平均流速为57.9cm/s,出现在夏季的18m层。（4）垂线平均余流为7.5~11.3 cm/s,春季最强冬季最弱;春季和冬季各层余流均为东向,夏季和秋季基本为东北向或北向。（5）观测海域海流受长江冲淡水、台湾暖流、季风、潮汐等动力作用的共同制约。     

南沙群岛海域混合层深度季节变化特征

基于南沙群岛海域综合科学考察11个航次的实测资料,研究了南沙群岛海域的混合层深度季节变化特征。研究结果表明,南沙群岛海域混合层深度存在明显的季节变化,并且与季风和海表热通量的变化密切相关。春季,风速较小且风向不稳定,海面得到的净热通量全年最大,上层水体层结稳定,混合层深度较小;夏季,南海西南季风盛行,上层为反气旋式环流,海面得到的净热通量减少,混合层呈加深的趋势;秋季,海面净热通量继续减少,混合层深度达到最大值;冬季,东北季风驱动下形成的上层气旋式环流引起深层冷水的上升,限制了混合层的加深。     

热带西太平洋主要流系的季节变化和年际变化

利用美国国家环境预报中心的太平洋海域１９８０～１９９５年四维同化资料,计算了棉兰老海流和与之有密切联系的北赤道流、北赤道逆流流量的年际变化和季节变化特征。由此得出以下结论：（１）棉兰老海流对北赤道逆流的初始流量贡献较大,是北赤道充的主要水源提供之一,棉兰老海流与黑湖在季节变化中存在反相关系;（２）棉兰老海流在厄尔诺年初期加强,在反厄尔尼诺期间减弱;（３）棉兰老海流的季节变化信号强于年际变化信号。     

秦皇岛港附近海域潮汐,波浪和海流特征

本文依据秦皇岛港区域潮汐、波浪和海流实测资料，对上述水动力要素作了初步探讨，进而揭示了港区附近海域潮汐、波浪和海流基本特征及其变化规律。     

好望角航道的海况和海冰的季节变化

西方详细分析了好望角航道的海洋状况,包括海流,海温,海雾和海冰。     

El Nino期间热带西太平洋海流对不同季节风场响应的数值模拟

本文试用二维绝热模式，用KWBC风场资料研究了1987年El Nino期间热带太平洋表层流系对冬、春、夏、秋季风场的响应特征。模拟结果表明：在1987年El Nino期间，赤道附近东向流加强了，西向流减弱了；冬季东向流距平比夏季强度大，纬向范围小且位置偏高；模拟海流及水位分布特征与中、美海－气相互作用热带西太平洋联合调查及Wyrtki的观测基本一致。     

南海北部春季海流的垂向变化

对南海北部一连续观测站的春季海流资料进行功率谱分析,潮流调和分析及统计分析,得到了南海北部春季海流垂向结构的基本特征为：（１）实测平均海流偏Ｗ向流动并随深度的增加稍作逆时针方向偏转,平均流速随深度的增加而减小,实测海流的日周期明显,在垂向上,近底层（３００ｍ）的功率谱峰值明显比其它水层的大,表明该层海流包含的日周期波动最强;（２）海区的日潮流相当强,其最大流速（Ｋｋ１＋Ｗｏ１）在近底层最大;日潮流     

1991-2011年东海黑潮PN断面流结构与季节变化分析

基于日本海洋信息中心提供的东海黑潮PN断面CTD资料,本文采用动力高度法计算了1991-2011年间90个航次的断面流速,并对流场结构、最大流速、流幅和流量进行了统计分析。结果表明:东海黑潮PN断面流场存在单核、双核、多核3种结构;其中单核结构出现的概率为50%,双核结构为39%,多核结构为11%。东海黑潮的流结构存在显著的季节变化:秋季多核结构所占的比重为4个季节最大,平均流核数最多;冬季主要为单核结构,平均流核数最少;夏季和春季则没有明显的倾向性,单核、双核、多核3种结构出现概率相近,平均流核数介于秋季和冬季之间。其次东海黑潮的流量也存在显著的季节变化:冬季与夏季最强,秋季最小,春季居中。最后东海黑潮的最大流速和流幅也存在季节变化:夏季最大,秋季最小,春季和冬季居中。     

浙江南部近海鱼类分类多样性研究

根据2015年11月至2016年8月浙江南部近海鱼类调查资料,采用纳尔逊分类系统整理鱼类物种组成,通过计算分类阶元包含指数(TINCL_i)、分类多样性指数(平均分类差异指数△+和分类差异变异指数∧+)分析浙南近海鱼类的分类多样性。调查结果共记录鱼类182种,分属18目78科130属。TINCL_i分析结果显示,浙南近海鱼类种类组成中,其目、科、属所包含的(科、属、种)、(属、种)和(种)的平均数目分别为(4.33、7.22、10.11)、(1.67、2.33)和(1.40)。浙江南部近海鱼类△+值和∧+值分别为62.9和77.0。浙江南部近海鱼类△+值小于高纬度的黄、渤海(66.4)和山东近海(66.1),大于低纬度的南沙群岛(56.6)、西沙群岛(60.2)和东沙群岛(55.2),呈现随着纬度降低鱼类△+值随之降低的规律。通过分析浙江南部近海鱼类的分类多样性,可以为浙江南部近海鱼类资源的可持续开发利用及保护提供重要的参考依据。     

黄海、东海表、上层实测流分析

根据迄今为止所获得的142套锚碇浮标和58套卫星跟踪漂流浮标的大范围测流资料，综合分析了黄海、东海表、上层环流。研究结果更加清晰、形象、直观地展示了黑潮及其向对马暖流的分支，台湾暖流的分叉，和黄海暖流、长江冲淡水及涡旋发达海区的若干主要特征。     

南黄海溶解氧的平面分布及其季节变化

根据中韩“黄海水循环及物质通量合作研究”项目1996～1997年现场调查获得的资料,首次对南黄海整个海域溶解氧的平面分布特征及其季节变化规律进行了探讨.对一些主要海洋过程如黄海暖流、台湾暖流、沿岸流、长江冲淡水、黄海冷水团及浮游植物的光合作用等对南黄海溶解氧含量分布的影响进行了讨论.     

南黄海浮游植物季节性变化的数值模拟与影响因子分析

用三维物理-生物耦合模式研究南黄海浮游植物(以叶绿素a为指标)的季节变化.对于物理模式采用Princeton ocean model(POM),对于生物模式考虑溶解无机营养盐(氮、磷、硅)、浮游植物、食草性浮游动物和碎屑.给定已知的初始场和外加边界强迫,模拟了观测到叶绿素a的主要时、空分布特征,如浮游植物的春、秋季水华和夏季次表层叶绿素a极大值现象等.研究表明,浮游植物春季水华最先发生于黄海中央海域,主要原因是该海域透明度较高,流速较小.春季水华开始于垂直对流减弱和层化开始形成之前(约3月底至4月上旬),显著地依赖水层的稳定性.水体层化以后(约5～9月)叶绿素a浓度高值区分布在南黄海的南部和锋区.夏季的南黄海中央海域,由于上混合层营养盐几乎耗尽,限制了浮游植物的生长,在紧贴温跃层下部的真光层,具有丰富的营养盐和合适的光照,次表层叶绿素a极大值得以形成.秋季(约9～11月份,略迟于海表面开始降温的时间,随地点不同而异)随垂直混合的增强,有利于营养盐向上输运,浮游植物出现一次较小的峰值.     

Distribution of phytoplankton in the East China Sea and the southern Yellow Sea in spring in relation to environmental variables and dimethylsulfide compounds

The coastal ecosystems are highly sensitive to climate change and are usually influenced by variations in phytoplankton communities and water physiochemical factors. In the present study, the phytoplankton community, chlorophyll a（Chl a） and their relationships with environmental variables and dimethylsulfide（DMS） and dimethylsulfoniopropionate（DMSP） were investigated in spring 2017（March 24 to April 16） in the East China Sea（26.0°–33.0°N, 120.0°–128.0°E） and southern Yellow Sea（31.0°–36.0°N, 12...     

南黄海和中国东海中挥发性卤代烃的分布与海气通量

Distributions and sea-to-air fluxes of five kinds of volatile halocarbons(VHCs) were studied in the southern Yellow Sea(SYS) and the East China Sea(ECS) in November 2007. The results showed that the concentrations of 1,1,1-trichloroethane(C2H3Cl3), 1,1-dichloroethene(C2H2Cl2), 1,1,2-trichloroethene(C2HCl3), trichloromethane(CHCl3) and tetrachloromethane(CCl4) in the surface water were 0.31–4.81, 2.75–21.3, 1.21–17.1, 5.02–233 and 0.045–4.47 pmol/L, respectively, with the average values of 1.89, 12.20, 6.93, 60.90 and 0.33 pmol/L. On the whole, the horizontal distributions of C2H3Cl3, C2H2Cl2 and CCl4 were affected mainly by anthropogenic activities, while C2HCl3 and CHCl3 were influenced by biological factors as well as anthropogenic activities. In the study area, the concentrations of VHCs(except C2HCl3) exhibited a decreasing trend from inshore to offshore sites, with the higher values occurring in the coastal waters. The sea-to-air fluxes of C2H3Cl3, C2HCl3, CHCl3 and CCl4 were calculated to be-56.00–(-5.68),-7.31–123.42, 148.00–1 309.31 and-83.32–(-1.53) nmol/(m2·d), respectively, with the average values of-6.77, 17.14, 183.38 and-21.27 nmol/(m2·d). Our data showed that the SYS and ECS in autumn was a sink for C2H3Cl3 and CCl4, while it was a source for C2HCl3 and CHCl3 in the atmosphere.     

Measurement of the current and spectral analysis on the continental shelf in the East China Sea

Direct measurements of current velocity and water temperature were undertaken at the mooring Sta. M (125°29.38' N, 31°49.70' E) on the continental shelf area in the East China Sea in June 1999 by R/V Xiangyanghong 14. The relationship between various time series of oceanic fluctuations is calculated by spectral analysis. The major results are as follows: (1) an average (u,v) of (6.9,-3.0 cm/s) at the 30 m depth is obtained during the 9-day observation, and that at the 45 m depth is (3.7,-1.1 cm/s), i. e., the mean flows are southeastward at both the 30 and 45 m depths;the currents become stronger gradually during the observation period; this may be mainly attributed to the transition of the tidal currents from neap to spring; (2)semidiurnal fluctuation is the most dominant in the current fluctuations, and rotates mainly clockwise; in the next place, there is also diurnal fluctuation;the local inertial period is close to the period of diurnal fluctuation, and an inertial motion is clockwise; thus, loca     

Measurement of the current and spectral analysis on the continental shelf in the East China Sea

Direct measurements of current velocity and water temperature were undertaken at the mooring Sta. M (125°29.38' N,31°49.70'E) on the continental shelf area in the East China Sea in June 1999 by R/V Xiangyanghong 14. The relationship between various time series of oceanic fluctuations is calculated by spectral analysis. The major results are as follows: (1) an average (u,v) of (6.9,-3.0 cm/s) at the 30 m depth is obtained during the 9-day observation, and that at the 45 m depth is (3.7,-1.1 cm/s), I. E., the mean flows are southeastward at both the 30 and 45 m depths;the currents become stronger gradually during the observation period; this may be mainly attributed to the transition of the tidal currents from neap to spring; (2)semidiurnal fluctuation is the most dominant in the current fluctuations, and rotates mainly clockwise; in the next place, there is also diurnal fluctuation;the local inertial period is close to the period of diurnal fluctuation, and an inertial motion is clockwise; thus, local inertial motion combines with diurnal fluctuation, and makes the spectral peaks in clockwise components much higher than those in counterclockwise ones;except for the fluctuations of above main periods, there is also the peak at 3 d period for counterclockwise components in the upper and lower layers; (3) the calculation of cross spectra between two time series of current velocities at the 30 and 45 m depths shows that both the current fluctuations at the 30 and 45 m depths are much alike, I. E.,they are synchro; this shows that the flow field here is rather vertically homogeneous; (4)power spectra of temperature time series at both the 30 and 45 m depths show that the semidiurnal peak is the most predominant, and the second highest peak is the diurnal period; besides spectral peaks at above periods, there are also obvious spectral peaks at 6.8 h and 2 d; (5)plots of temperature time series at 16,30,35,45 and 50 m depths show that the temporal variations of temperature at these depths are synchro, which are like those in the velocity field; temperature records also show a gradual rise in temperature, which are also like those in the velocity field.     

东海黑潮活跃区表层流场的半年内时间尺度变化研究

利用高时空分辨率的资料,对东海黑潮表层海流的半年内时间尺度变化特征进行了分析研究,得到主要以下结论:(1)东海黑潮表层海流在台湾东北海区和吐噶喇海峡附近海区存在着最为显著的变化;(2)那里的表层海流都存在半年内时间尺度的变化,其谱峰主要在50~70d及90~140d两个频段内,两个准周期变化的基本特征都是异常气旋涡和反气旋涡的准周期转换;(3)异常气旋涡和反气旋涡的活动都与东海黑潮在两个海区的流轴变化相联系,气旋涡与黑潮流轴在该海区的向东南退缩相伴,而反气旋涡与黑潮流轴在该海区的向西北推进相伴;(4)初步分析表明,在台湾东北海域导致50~70d变化的异常涡旋主要源于黑潮自身存在的中尺度过程,而90~140d的变化则主要受从台湾以东传来的中尺度涡影响。类似地,吐噶喇海峡附近的黑潮海流同样在50~70d及90~140d两个频段内存在显著的准周期变化,回归分析表明,导致50~70d变化主要源于上游黑潮海流的中尺度过程,而90~140d的变化则主要受琉球群岛以东传来的中尺度涡影响。